Mg 2؉ ions are very effective at stabilizing tertiary structures in RNAs. In most cases, folding of an RNA is so strongly coupled to its interactions with Mg 2؉ that it is difficult to separate free energies of Mg 2؉ -RNA interactions from the intrinsic free energy of RNA folding. To devise quantitative models accounting for this phenomenon of Mg 2؉ -induced RNA folding, it is necessary to independently determine Mg 2؉ -RNA interaction free energies for folded and unfolded RNA forms. In this work, the energetics of Mg 2؉ -RNA interactions are derived from an assay that measures the effective concentration of Mg 2؉ in the presence of RNA. These measurements are used with other measures of RNA stability to develop an overall picture of the energetics of Mg 2؉ -induced RNA folding. Two different RNAs are discussed, a pseudoknot and an rRNA fragment. Both RNAs interact strongly with Mg 2؉ when partially unfolded, but the two folded RNAs differ dramatically in their inherent stability in the absence of Mg 2؉ and in the free energy of their interactions with Mg 2؉ . From these results, it appears that any comprehensive framework for understanding Mg 2؉ -induced stabilization of RNA will have to (i) take into account the interactions of ions with the partially unfolded RNAs and (ii) identify factors responsible for the widely different strengths with which folded tertiary structures interact with Mg 2؉ .cations ͉ ion interaction coefficients ͉ Wyman linkage relations M g 2ϩ ions strongly stabilize RNA tertiary structures under conditions that only weakly affect RNA secondary structure stability, a phenomenon first studied in the folding of transfer RNA (1, 2). Although the sensitivity of RNA folding to Mg 2ϩ has been amply documented for many RNAs, it is still unknown how this sensitivity is quantitatively related to the strengths of Mg 2ϩ -RNA interactions. Thus, for most RNAs, the magnitude of the intrinsic RNA instability is unknown, nor is it known how much more favorably Mg 2ϩ interacts with the native RNA structure than with structures from which folding takes place. Lacking this fundamental overview of Mg 2ϩ -RNA interaction free energies, it has not been possible to carry out extensive evaluations of theoretical models that seek to explain Mg 2ϩ -induced RNA folding in terms of the underlying physical interactions (3, 4).In this article, we parse the tertiary folding of two different RNAs into the intrinsic free energy of folding in the absence of Mg 2ϩ and the free energies of Mg 2ϩ interactions with folded and partially folded states. To obtain the relevant free energies, we devised a practical experimental method for measuring the effect of RNA on Mg 2ϩ ion activities and derived the equations necessary for extracting Mg 2ϩ -RNA interaction free energies from the experimental data. The two RNAs have vastly different stabilities in the absence of Mg 2ϩ and correspondingly large differences in the favorable interactions of the native RNA structures with Mg 2ϩ . Clearly, different RNAs use different strategies ...